Method of processing a workpiece in a plasma reactor with variable height ground return path to control plasma ion density uniformity

Abstract

A method for processing a workpiece in a plasma reactor chamber includes coupling RF power at a first VHF frequency f1 to a plasma via one of the electrodes of the chamber, and providing a center ground return path for RF current passing directly between the ceiling electrode and the workpiece support electrode for the frequency f1. The method further includes providing a variable height edge ground annular element and providing a ground return path through the edge ground annular element for the frequency f1. The method controls the uniformity of plasma ion density distribution by controlling the distance between the variable height edge ground annular element and one of: (a) height of ceiling electrode or (b) height of workpiece support electrode.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS[0001]This application claims the benefit of U.S. Provisional Application Ser. No. 60 / 898,632, filed Jan. 30, 2007.BACKGROUND[0002]Embodiments of the present invention concern a capacitively coupled plasma source for processing a workpiece such as a semiconductor wafer. A capacitively coupled plasma source comprises a ceiling electrode that is driven at a very high frequency (VHF) frequency over 110 MHz which can produce a high density plasma at a relatively low voltage. A capacitively coupled plasma source can further produce a low electrode potential for low electrode erosion, and permits the ion energy at the wafer surface to be limited to a low level if desired, while operating over a wide range of plasma density (very low to very high plasma ion density). One problem inherent in such a plasma source is that the ceiling electrode exhibits radial transmission line effects and loading due to the effective dielectric constant of the plasma. Fo...

AI Technical Summary

Benefits of technology

[0005]A method is provided for processing a workpiece in a plasma reactor chamber having at least a ceiling electrode and a workpiece support electrode. The method includes coupling RF power at a first VHF frequency f1 to a plasma via one of the electrodes of the chamber, and providing a center ground return path for RF current passing directly between the ceiling electrode and the workpiece support electrode for the frequency f1. The method further includes providing a variable height edge ground annular element and providing a ground return path through the edge ground annular element for the frequency f1. The method controls the uniformity of plasma ion density distribution by controlling the distance between the variable height edge ground annular element and one of: (a) height of ceiling electrode or (b) height of workpiece support electrode.

[0006]In one embodiment, the method further includes adjusting the impedance of the center ground return path corresponding to the frequency f1 so as to increase or decrease the tendency of the RF power at f1 to produce a center-high non-uniformity in plasma ion density distribution.

Problems solved by technology

One problem inherent in such a plasma source is that the ceiling electrode exhibits radial transmission line effects and loading due to the effective dielectric constant of the plasma.

Therefore, the RF field varies significantly across the surface of the ceiling electrode, giving rise to process non-uniformities at the wafer surface.

For a plasma with an effective dielectric constant greater than 1, the effective wavelength is reduced to less than the ceiling electrode diameter, worsening the non-uniformity of the RF field, making processing non-uniformities across the wafer surface worse.

For an etch process, this may produce a non-uniform edge low etch rate distribution across the wafer surface.

One problem with this approach is that a center-high non-uniformity of the source may be beyond the corrective capability of magnetic steering.

Another problem with this approach can be electrical charging damage of the workpiece if the magnetic flux density is too high.

The net effect is to reduce the effect of the dielectric constant of the plasma, thereby reducing the non-uniformity of the RF field.

However, a high plasma bias voltage is not desirable in some other types of plasma processes.

The worst non-uniformities appear in processes employing the lowest plasma bias voltage.

Such approaches are complicated by the fact that other process conditions dictated by the process recipe have as great an effect upon plasma distribution as either magnetic steering or bias (sheath) voltage.

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